# -*- coding: utf-8 -*- ''' *GSASIIstrMain: main structure routine* --------------------------------------- ''' ########### SVN repository information ################### # $Date: 2017-02-23 19:26:52 +0000 (Thu, 23 Feb 2017) $ # $Author: vondreele $ # $Revision: 2721 $ # $URL: trunk/GSASIIstrMain.py $ # $Id: GSASIIstrMain.py 2721 2017-02-23 19:26:52Z vondreele $ ########### SVN repository information ################### import sys import os.path as ospath import time import math import copy import numpy as np import numpy.linalg as nl import scipy.optimize as so import GSASIIpath GSASIIpath.SetVersionNumber("$Revision: 2721 $") import GSASIIlattice as G2lat import GSASIIspc as G2spc import GSASIImapvars as G2mv import GSASIImath as G2mth import GSASIIstrIO as G2stIO import GSASIIstrMath as G2stMth import GSASIIobj as G2obj sind = lambda x: np.sin(x*np.pi/180.) cosd = lambda x: np.cos(x*np.pi/180.) tand = lambda x: np.tan(x*np.pi/180.) asind = lambda x: 180.*np.arcsin(x)/np.pi acosd = lambda x: 180.*np.arccos(x)/np.pi atan2d = lambda y,x: 180.*np.arctan2(y,x)/np.pi ateln2 = 8.0*math.log(2.0) DEBUG = True def RefineCore(Controls,Histograms,Phases,restraintDict,rigidbodyDict,parmDict,varyList, calcControls,pawleyLookup,ifPrint,printFile,dlg): 'Core optimization routines, shared between SeqRefine and Refine' # print 'current',varyList # for item in parmDict: print item,parmDict[item] ######### show dict just before refinement G2mv.Map2Dict(parmDict,varyList) Rvals = {} while True: begin = time.time() values = np.array(G2stMth.Dict2Values(parmDict, varyList)) # test code to compute GOF and save for external repeat #args = ([Histograms,Phases,restraintDict,rigidbodyDict],parmDict,varyList,calcControls,pawleyLookup,dlg) #print '*** before fit chi**2',np.sum(G2stMth.errRefine(values,*args)**2) #fl = open('beforeFit.cpickle','wb') #import cPickle #cPickle.dump(values,fl,1) #cPickle.dump(args[:-1],fl,1) #fl.close() Ftol = Controls['min dM/M'] Factor = Controls['shift factor'] if 'Jacobian' in Controls['deriv type']: result = so.leastsq(G2stMth.errRefine,values,Dfun=G2stMth.dervRefine,full_output=True, ftol=Ftol,col_deriv=True,factor=Factor, args=([Histograms,Phases,restraintDict,rigidbodyDict],parmDict,varyList,calcControls,pawleyLookup,dlg)) ncyc = int(result[2]['nfev']/2) elif 'Hessian' in Controls['deriv type']: Lamda = Controls.get('Marquardt',-3) maxCyc = Controls['max cyc'] result = G2mth.HessianLSQ(G2stMth.errRefine,values,Hess=G2stMth.HessRefine,ftol=Ftol,maxcyc=maxCyc,Print=ifPrint,lamda=Lamda, args=([Histograms,Phases,restraintDict,rigidbodyDict],parmDict,varyList,calcControls,pawleyLookup,dlg)) ncyc = result[2]['num cyc']+1 Rvals['lamMax'] = result[2]['lamMax'] Controls['Marquardt'] = -3 #reset to default else: #'numeric' result = so.leastsq(G2stMth.errRefine,values,full_output=True,ftol=Ftol,epsfcn=1.e-8,factor=Factor, args=([Histograms,Phases,restraintDict,rigidbodyDict],parmDict,varyList,calcControls,pawleyLookup,dlg)) ncyc = 1 if len(varyList): ncyc = int(result[2]['nfev']/len(varyList)) # table = dict(zip(varyList,zip(values,result[0],(result[0]-values)))) # for item in table: print item,table[item] #useful debug - are things shifting? runtime = time.time()-begin Rvals['converged'] = result[2].get('Converged') Rvals['DelChi2'] = result[2].get('DelChi2',-1.) Rvals['chisq'] = np.sum(result[2]['fvec']**2) G2stMth.Values2Dict(parmDict, varyList, result[0]) G2mv.Dict2Map(parmDict,varyList) Rvals['Nobs'] = Histograms['Nobs'] Rvals['Rwp'] = np.sqrt(Rvals['chisq']/Histograms['sumwYo'])*100. #to % Rvals['GOF'] = np.sqrt(Rvals['chisq']/(Histograms['Nobs']-len(varyList))) print >>printFile,' Number of function calls:',result[2]['nfev'], \ ' No. of observations: ',Histograms['Nobs'],' No. of parameters: ',len(varyList), \ ' User rejected: ',Histograms['Nrej'],' Sp. gp. extinct: ',Histograms['Next'] print >>printFile,' Refinement time = %8.3fs, %8.3fs/cycle, for %d cycles'%(runtime,runtime/ncyc,ncyc) print >>printFile,' wR = %7.2f%%, chi**2 = %12.6g, GOF = %6.2f'%(Rvals['Rwp'],Rvals['chisq'],Rvals['GOF']) IfOK = True try: covMatrix = result[1]*Rvals['GOF']**2 sig = np.sqrt(np.diag(covMatrix)) if np.any(np.isnan(sig)): print '*** Least squares aborted - some invalid esds possible ***' # table = dict(zip(varyList,zip(values,result[0],(result[0]-values)/sig))) # for item in table: print item,table[item] #useful debug - are things shifting? break #refinement succeeded - finish up! except TypeError: #result[1] is None on singular matrix IfOK = False if not len(varyList): covMatrix = [] sig = [] break print '**** Refinement failed - singular matrix ****' if 'Hessian' in Controls['deriv type']: num = len(varyList)-1 for i,val in enumerate(np.flipud(result[2]['psing'])): if val: print 'Removing parameter: ',varyList[num-i] del(varyList[num-i]) else: Ipvt = result[2]['ipvt'] for i,ipvt in enumerate(Ipvt): if not np.sum(result[2]['fjac'],axis=1)[i]: print 'Removing parameter: ',varyList[ipvt-1] del(varyList[ipvt-1]) break G2stMth.GetFobsSq(Histograms,Phases,parmDict,calcControls) return IfOK,Rvals,result,covMatrix,sig def Refine(GPXfile,dlg): 'Global refinement -- refines to minimize against all histograms' import pytexture as ptx ptx.pyqlmninit() #initialize fortran arrays for spherical harmonics printFile = open(ospath.splitext(GPXfile)[0]+'.lst','w') G2stIO.ShowBanner(printFile) varyList = [] parmDict = {} G2mv.InitVars() Controls = G2stIO.GetControls(GPXfile) G2stIO.ShowControls(Controls,printFile) calcControls = {} calcControls.update(Controls) constrDict,fixedList = G2stIO.GetConstraints(GPXfile) restraintDict = G2stIO.GetRestraints(GPXfile) Histograms,Phases = G2stIO.GetUsedHistogramsAndPhases(GPXfile) if not Phases: print ' *** ERROR - you have no phases to refine! ***' print ' *** Refine aborted ***' return False,'No phases' if not Histograms: print ' *** ERROR - you have no data to refine with! ***' print ' *** Refine aborted ***' return False,'No data' rigidbodyDict = G2stIO.GetRigidBodies(GPXfile) rbIds = rigidbodyDict.get('RBIds',{'Vector':[],'Residue':[]}) rbVary,rbDict = G2stIO.GetRigidBodyModels(rigidbodyDict,pFile=printFile) Natoms,atomIndx,phaseVary,phaseDict,pawleyLookup,FFtables,BLtables,MFtables,maxSSwave = \ G2stIO.GetPhaseData(Phases,restraintDict,rbIds,pFile=printFile) calcControls['atomIndx'] = atomIndx calcControls['Natoms'] = Natoms calcControls['FFtables'] = FFtables calcControls['BLtables'] = BLtables calcControls['MFtables'] = MFtables calcControls['maxSSwave'] = maxSSwave hapVary,hapDict,controlDict = G2stIO.GetHistogramPhaseData(Phases,Histograms,pFile=printFile) TwConstr,TwFixed = G2stIO.makeTwinFrConstr(Phases,Histograms,hapVary) constrDict += TwConstr fixedList += TwFixed calcControls.update(controlDict) histVary,histDict,controlDict = G2stIO.GetHistogramData(Histograms,pFile=printFile) calcControls.update(controlDict) varyList = rbVary+phaseVary+hapVary+histVary parmDict.update(rbDict) parmDict.update(phaseDict) parmDict.update(hapDict) parmDict.update(histDict) G2stIO.GetFprime(calcControls,Histograms) # do constraint processing varyListStart = tuple(varyList) # save the original varyList before dependent vars are removed try: groups,parmlist = G2mv.GroupConstraints(constrDict) G2mv.GenerateConstraints(groups,parmlist,varyList,constrDict,fixedList,parmDict) #print G2mv.VarRemapShow(varyList) #print 'DependentVars',G2mv.GetDependentVars() #print 'IndependentVars',G2mv.GetIndependentVars() except: print ' *** ERROR - your constraints are internally inconsistent ***' #errmsg, warnmsg = G2mv.CheckConstraints(varyList,constrDict,fixedList) #print 'Errors',errmsg #if warnmsg: print 'Warnings',warnmsg return False,' Constraint error' # print G2mv.VarRemapShow(varyList) ifPrint = True print >>printFile,'\n Refinement results:' print >>printFile,135*'-' try: covData = {} IfOK,Rvals,result,covMatrix,sig = RefineCore(Controls,Histograms,Phases,restraintDict, rigidbodyDict,parmDict,varyList,calcControls,pawleyLookup,ifPrint,printFile,dlg) sigDict = dict(zip(varyList,sig)) newCellDict = G2stMth.GetNewCellParms(parmDict,varyList) newAtomDict = G2stMth.ApplyXYZshifts(parmDict,varyList) covData = {'variables':result[0],'varyList':varyList,'sig':sig,'Rvals':Rvals, 'varyListStart':varyListStart, 'covMatrix':covMatrix,'title':GPXfile,'newAtomDict':newAtomDict, 'newCellDict':newCellDict,'freshCOV':True} # add the uncertainties into the esd dictionary (sigDict) sigDict.update(G2mv.ComputeDepESD(covMatrix,varyList,parmDict)) G2mv.PrintIndependentVars(parmDict,varyList,sigDict,pFile=printFile) G2stMth.ApplyRBModels(parmDict,Phases,rigidbodyDict,True) G2stIO.SetRigidBodyModels(parmDict,sigDict,rigidbodyDict,printFile) G2stIO.SetPhaseData(parmDict,sigDict,Phases,rbIds,covData,restraintDict,printFile) G2stIO.SetHistogramPhaseData(parmDict,sigDict,Phases,Histograms,calcControls['FFtables'],pFile=printFile) G2stIO.SetHistogramData(parmDict,sigDict,Histograms,calcControls['FFtables'],pFile=printFile) G2stIO.SetUsedHistogramsAndPhases(GPXfile,Histograms,Phases,rigidbodyDict,covData) printFile.close() print ' Refinement results are in file: '+ospath.splitext(GPXfile)[0]+'.lst' print ' ***** Refinement successful *****' except G2obj.G2Exception,Msg: printFile.close() return False,Msg.msg #for testing purposes!!! if DEBUG: #needs: values,HistoPhases,parmDict,varylist,calcControls,pawleyLookup import cPickle fl = open('testDeriv.dat','wb') cPickle.dump(result[0],fl,1) cPickle.dump([Histograms,Phases,restraintDict,rigidbodyDict],fl,1) cPickle.dump([constrDict,fixedList,G2mv.GetDependentVars()],fl,1) cPickle.dump(parmDict,fl,1) cPickle.dump(varyList,fl,1) cPickle.dump(calcControls,fl,1) cPickle.dump(pawleyLookup,fl,1) fl.close() if dlg: return True,Rvals def phaseCheck(phaseVary,Phases,histogram): ''' Removes unused parameters from phase varylist if phase not in histogram ''' pIds = [] for phase in Phases: if Phases[phase]['Histograms'][histogram]['Use']: pIds.append(str(Phases[phase]['pId'])) return [item for item in phaseVary if item.split(':')[0] in pIds] def SeqRefine(GPXfile,dlg): '''Perform a sequential refinement -- cycles through all selected histgrams, one at a time ''' import pytexture as ptx ptx.pyqlmninit() #initialize fortran arrays for spherical harmonics printFile = open(ospath.splitext(GPXfile)[0]+'.lst','w') print 'Starting Sequential Refinement' G2stIO.ShowBanner(printFile) Controls = G2stIO.GetControls(GPXfile) G2stIO.ShowControls(Controls,printFile,SeqRef=True) restraintDict = G2stIO.GetRestraints(GPXfile) Histograms,Phases = G2stIO.GetUsedHistogramsAndPhases(GPXfile) if not Phases: print ' *** ERROR - you have no phases to refine! ***' print ' *** Refine aborted ***' return False,'No phases' if not Histograms: print ' *** ERROR - you have no data to refine with! ***' print ' *** Refine aborted ***' return False,'No data' rigidbodyDict = G2stIO.GetRigidBodies(GPXfile) rbIds = rigidbodyDict.get('RBIds',{'Vector':[],'Residue':[]}) rbVary,rbDict = G2stIO.GetRigidBodyModels(rigidbodyDict,pFile=printFile) Natoms,atomIndx,phaseVary,phaseDict,pawleyLookup,FFtables,BLtables,MFtables,maxSSwave = \ G2stIO.GetPhaseData(Phases,restraintDict,rbIds,False,printFile,seqRef=True) for item in phaseVary: if '::A0' in item: print '**** WARNING - lattice parameters should not be refined in a sequential refinement ****' print '**** instead use the Dij parameters for each powder histogram ****' return False,'Lattice parameter refinement error - see console message' if '::C(' in item: print '**** WARNING - phase texture parameters should not be refined in a sequential refinement ****' print '**** instead use the C(L,N) parameters for each powder histogram ****' return False,'Phase texture refinement error - see console message' if 'Seq Data' in Controls: histNames = Controls['Seq Data'] else: histNames = G2stIO.GetHistogramNames(GPXfile,['PWDR',]) if Controls.get('Reverse Seq'): histNames.reverse() SeqResult = G2stIO.GetSeqResult(GPXfile) # SeqResult = {'SeqPseudoVars':{},'SeqParFitEqList':[]} makeBack = True Histo = {} NewparmDict = {} for ihst,histogram in enumerate(histNames): print('Refining with '+str(histogram)) ifPrint = False if dlg: dlg.SetTitle('Residual for histogram '+str(ihst)) calcControls = {} calcControls['atomIndx'] = atomIndx calcControls['Natoms'] = Natoms calcControls['FFtables'] = FFtables calcControls['BLtables'] = BLtables calcControls['MFtables'] = MFtables calcControls['maxSSwave'] = maxSSwave if histogram not in Histograms: print("Error: not found!") continue redphaseVary = phaseCheck(phaseVary,Phases,histogram) Histo = {histogram:Histograms[histogram],} hapVary,hapDict,controlDict = G2stIO.GetHistogramPhaseData(Phases,Histo,Print=False) calcControls.update(controlDict) histVary,histDict,controlDict = G2stIO.GetHistogramData(Histo,False) calcControls.update(controlDict) varyList = rbVary+redphaseVary+hapVary+histVary # if not ihst: # save the initial vary list, but without histogram numbers on parameters saveVaryList = varyList[:] for i,item in enumerate(saveVaryList): items = item.split(':') if items[1]: items[1] = '' item = ':'.join(items) saveVaryList[i] = item if not ihst: SeqResult['varyList'] = saveVaryList else: SeqResult['varyList'] = list(set(SeqResult['varyList']+saveVaryList)) parmDict = {} parmDict.update(phaseDict) parmDict.update(hapDict) parmDict.update(histDict) if Controls['Copy2Next']: parmDict.update(NewparmDict) G2stIO.GetFprime(calcControls,Histo) # do constraint processing #reload(G2mv) # debug G2mv.InitVars() constrDict,fixedList = G2stIO.GetConstraints(GPXfile) varyListStart = tuple(varyList) # save the original varyList before dependent vars are removed try: groups,parmlist = G2mv.GroupConstraints(constrDict) G2mv.GenerateConstraints(groups,parmlist,varyList,constrDict,fixedList,parmDict,SeqHist=ihst) constraintInfo = (groups,parmlist,constrDict,fixedList,ihst) except: print ' *** ERROR - your constraints are internally inconsistent ***' #errmsg, warnmsg = G2mv.CheckConstraints(varyList,constrDict,fixedList) #print 'Errors',errmsg #if warnmsg: print 'Warnings',warnmsg return False,' Constraint error' #print G2mv.VarRemapShow(varyList) if not ihst: # first histogram to refine against firstVaryList = [] for item in varyList: items = item.split(':') if items[1]: items[1] = '' item = ':'.join(items) firstVaryList.append(item) newVaryList = firstVaryList else: newVaryList = [] for item in varyList: items = item.split(':') if items[1]: items[1] = '' item = ':'.join(items) newVaryList.append(item) if newVaryList != firstVaryList and Controls['Copy2Next']: # variable lists are expected to match between sequential refinements when Copy2Next is on print '**** ERROR - variable list for this histogram does not match previous' print ' Copy of variables is not possible' print '\ncurrent histogram',histogram,'has',len(newVaryList),'variables' combined = list(set(firstVaryList+newVaryList)) c = [var for var in combined if var not in newVaryList] p = [var for var in combined if var not in firstVaryList] line = 'Variables in previous but not in current: ' if c: for var in c: if len(line) > 100: print line line = ' ' line += var + ', ' else: line += 'none' print line print '\nPrevious refinement has',len(firstVaryList),'variables' line = 'Variables in current but not in previous: ' if p: for var in p: if len(line) > 100: print line line = ' ' line += var + ', ' else: line += 'none' print line return False,line ifPrint = False print >>printFile,'\n Refinement results for histogram: v'+histogram print >>printFile,135*'-' try: IfOK,Rvals,result,covMatrix,sig = RefineCore(Controls,Histo,Phases,restraintDict, rigidbodyDict,parmDict,varyList,calcControls,pawleyLookup,ifPrint,printFile,dlg) print ' wR = %7.2f%%, chi**2 = %12.6g, reduced chi**2 = %6.2f, last delta chi = %.4f'%( Rvals['Rwp'],Rvals['chisq'],Rvals['GOF']**2,Rvals['DelChi2']) # add the uncertainties into the esd dictionary (sigDict) sigDict = dict(zip(varyList,sig)) # the uncertainties for dependent constrained parms into the esd dict sigDict.update(G2mv.ComputeDepESD(covMatrix,varyList,parmDict)) # a dict with values & esds for dependent (constrained) parameters - avoid extraneous holds depParmDict = {i:(parmDict[i],sigDict[i]) for i in varyListStart if i in sigDict and i not in varyList} newCellDict = copy.deepcopy(G2stMth.GetNewCellParms(parmDict,varyList)) newAtomDict = copy.deepcopy(G2stMth.ApplyXYZshifts(parmDict,varyList)) histRefData = { 'variables':result[0],'varyList':varyList,'sig':sig,'Rvals':Rvals, 'varyListStart':varyListStart, 'covMatrix':covMatrix,'title':histogram,'newAtomDict':newAtomDict, 'newCellDict':newCellDict,'depParmDict':depParmDict, 'constraintInfo':constraintInfo, 'parmDict':parmDict} SeqResult[histogram] = histRefData G2stMth.ApplyRBModels(parmDict,Phases,rigidbodyDict,True) # G2stIO.SetRigidBodyModels(parmDict,sigDict,rigidbodyDict,printFile) G2stIO.SetHistogramPhaseData(parmDict,sigDict,Phases,Histo,None,ifPrint,printFile) G2stIO.SetHistogramData(parmDict,sigDict,Histo,None,ifPrint,printFile) G2stIO.SetUsedHistogramsAndPhases(GPXfile,Histo,Phases,rigidbodyDict,histRefData,makeBack) makeBack = False NewparmDict = {} # make dict of varied parameters in current histogram, renamed to # next histogram, for use in next refinement. if Controls['Copy2Next'] and ihst < len(histNames)-1: hId = Histo[histogram]['hId'] # current histogram nexthId = Histograms[histNames[ihst+1]]['hId'] for parm in set(list(varyList)+list(varyListStart)): items = parm.split(':') if len(items) < 3: continue if str(hId) in items[1]: items[1] = str(nexthId) newparm = ':'.join(items) NewparmDict[newparm] = parmDict[parm] except G2obj.G2Exception,Msg: printFile.close() print ' ***** Refinement aborted *****' return False,Msg.msg if Controls.get('Reverse Seq'): histNames.reverse() SeqResult['histNames'] = histNames G2stIO.SetSeqResult(GPXfile,Histograms,SeqResult) printFile.close() print ' Sequential refinement results are in file: '+ospath.splitext(GPXfile)[0]+'.lst' print ' ***** Sequential refinement successful *****' return True,'Success' def RetDistAngle(DisAglCtls,DisAglData): '''Compute and return distances and angles :param dict DisAglCtls: contains distance/angle radii usually defined using :func:`GSASIIgrid.DisAglDialog` :param dict DisAglData: contains phase data: Items 'OrigAtoms' and 'TargAtoms' contain the atoms to be used for distance/angle origins and atoms to be used as targets. Item 'SGData' has the space group information (see :ref:`Space Group object`) :returns: AtomLabels,DistArray,AngArray where: **AtomLabels** is a dict of atom labels, keys are the atom number **DistArray** is a dict keyed by the origin atom number where the value is a list of distance entries. The value for each distance is a list containing: 0) the target atom number (int); 1) the unit cell offsets added to x,y & z (tuple of int values) 2) the symmetry operator number (which may be modified to indicate centering and center of symmetry) 3) an interatomic distance in A (float) 4) an uncertainty on the distance in A or 0.0 (float) **AngArray** is a dict keyed by the origin (central) atom number where the value is a list of angle entries. The value for each angle entry consists of three values: 0) a distance item reference for one neighbor (int) 1) a distance item reference for a second neighbor (int) 2) a angle, uncertainty pair; the s.u. may be zero (tuple of two floats) The AngArray distance reference items refer directly to the index of the items in the DistArray item for the list of distances for the central atom. ''' import numpy.ma as ma SGData = DisAglData['SGData'] Cell = DisAglData['Cell'] Amat,Bmat = G2lat.cell2AB(Cell[:6]) covData = {} if 'covData' in DisAglData: covData = DisAglData['covData'] covMatrix = covData['covMatrix'] varyList = covData['varyList'] pfx = str(DisAglData['pId'])+'::' Factor = DisAglCtls['Factors'] Radii = dict(zip(DisAglCtls['AtomTypes'],zip(DisAglCtls['BondRadii'],DisAglCtls['AngleRadii']))) indices = (-2,-1,0,1,2) Units = np.array([[h,k,l] for h in indices for k in indices for l in indices]) origAtoms = DisAglData['OrigAtoms'] targAtoms = DisAglData['TargAtoms'] AtomLabels = {} for Oatom in origAtoms: AtomLabels[Oatom[0]] = Oatom[1] for Oatom in targAtoms: AtomLabels[Oatom[0]] = Oatom[1] DistArray = {} AngArray = {} for Oatom in origAtoms: DistArray[Oatom[0]] = [] AngArray[Oatom[0]] = [] OxyzNames = '' IndBlist = [] Dist = [] Vect = [] VectA = [] angles = [] for Tatom in targAtoms: Xvcov = [] TxyzNames = '' if 'covData' in DisAglData: OxyzNames = [pfx+'dAx:%d'%(Oatom[0]),pfx+'dAy:%d'%(Oatom[0]),pfx+'dAz:%d'%(Oatom[0])] TxyzNames = [pfx+'dAx:%d'%(Tatom[0]),pfx+'dAy:%d'%(Tatom[0]),pfx+'dAz:%d'%(Tatom[0])] Xvcov = G2mth.getVCov(OxyzNames+TxyzNames,varyList,covMatrix) result = G2spc.GenAtom(Tatom[3:6],SGData,False,Move=False) BsumR = (Radii[Oatom[2]][0]+Radii[Tatom[2]][0])*Factor[0] AsumR = (Radii[Oatom[2]][1]+Radii[Tatom[2]][1])*Factor[1] for Txyz,Top,Tunit in result: Dx = (Txyz-np.array(Oatom[3:6]))+Units dx = np.inner(Amat,Dx) dist = ma.masked_less(np.sqrt(np.sum(dx**2,axis=0)),0.5) IndB = ma.nonzero(ma.masked_greater(dist-BsumR,0.)) if np.any(IndB): for indb in IndB: for i in range(len(indb)): if str(dx.T[indb][i]) not in IndBlist: IndBlist.append(str(dx.T[indb][i])) unit = Units[indb][i] tunit = (unit[0]+Tunit[0],unit[1]+Tunit[1],unit[2]+Tunit[2]) pdpx = G2mth.getDistDerv(Oatom[3:6],Tatom[3:6],Amat,unit,Top,SGData) sig = 0.0 if len(Xvcov): sig = np.sqrt(np.inner(pdpx,np.inner(pdpx,Xvcov))) Dist.append([Oatom[0],Tatom[0],tunit,Top,ma.getdata(dist[indb])[i],sig]) if (Dist[-1][-2]-AsumR) <= 0.: Vect.append(dx.T[indb][i]/Dist[-1][-2]) VectA.append([OxyzNames,np.array(Oatom[3:6]),TxyzNames,np.array(Tatom[3:6]),unit,Top]) else: Vect.append([0.,0.,0.]) VectA.append([]) for D in Dist: DistArray[Oatom[0]].append(D[1:]) Vect = np.array(Vect) angles = np.zeros((len(Vect),len(Vect))) angsig = np.zeros((len(Vect),len(Vect))) for i,veca in enumerate(Vect): if np.any(veca): for j,vecb in enumerate(Vect): if np.any(vecb): angles[i][j],angsig[i][j] = G2mth.getAngSig(VectA[i],VectA[j],Amat,SGData,covData) if i <= j: continue AngArray[Oatom[0]].append((i,j, G2mth.getAngSig(VectA[i],VectA[j],Amat,SGData,covData))) return AtomLabels,DistArray,AngArray def PrintDistAngle(DisAglCtls,DisAglData,out=sys.stdout): '''Print distances and angles :param dict DisAglCtls: contains distance/angle radii usually defined using :func:`GSASIIgrid.DisAglDialog` :param dict DisAglData: contains phase data: Items 'OrigAtoms' and 'TargAtoms' contain the atoms to be used for distance/angle origins and atoms to be used as targets. Item 'SGData' has the space group information (see :ref:`Space Group object`) :param file out: file object for output. Defaults to sys.stdout. ''' def MyPrint(s): out.write(s+'\n') # print(s,file=out) # use in Python 3 def ShowBanner(name): MyPrint(80*'*') MyPrint(' Interatomic Distances and Angles for phase '+name) MyPrint((80*'*')+'\n') ShowBanner(DisAglCtls['Name']) SGData = DisAglData['SGData'] SGtext,SGtable = G2spc.SGPrint(SGData) for line in SGtext: MyPrint(line) if len(SGtable) > 1: for i,item in enumerate(SGtable[::2]): if 2*i+1 == len(SGtable): line = ' %s'%(item.ljust(30)) else: line = ' %s %s'%(item.ljust(30),SGtable[2*i+1].ljust(30)) MyPrint(line) else: MyPrint(' ( 1) %s'%(SGtable[0])) #triclinic case Cell = DisAglData['Cell'] Amat,Bmat = G2lat.cell2AB(Cell[:6]) covData = {} if 'covData' in DisAglData: covData = DisAglData['covData'] pfx = str(DisAglData['pId'])+'::' A = G2lat.cell2A(Cell[:6]) cellSig = G2stIO.getCellEsd(pfx,SGData,A,covData) names = [' a = ',' b = ',' c = ',' alpha = ',' beta = ',' gamma = ',' Volume = '] valEsd = [G2mth.ValEsd(Cell[i],cellSig[i],True) for i in range(7)] line = '\n Unit cell:' for name,vals in zip(names,valEsd): line += name+vals MyPrint(line) else: MyPrint('\n Unit cell: a = '+('%.5f'%Cell[0])+' b = '+('%.5f'%Cell[1])+' c = '+('%.5f'%Cell[2])+ ' alpha = '+('%.3f'%Cell[3])+' beta = '+('%.3f'%Cell[4])+' gamma = '+ ('%.3f'%Cell[5])+' Volume = '+('%.3f'%Cell[6])) AtomLabels,DistArray,AngArray = RetDistAngle(DisAglCtls,DisAglData) origAtoms = DisAglData['OrigAtoms'] for Oatom in origAtoms: i = Oatom[0] Dist = DistArray[i] nDist = len(Dist) angles = np.zeros((nDist,nDist)) angsig = np.zeros((nDist,nDist)) for k,j,tup in AngArray[i]: angles[k][j],angsig[k][j] = angles[j][k],angsig[j][k] = tup line = '' for i,x in enumerate(Oatom[3:6]): line += ('%12.5f'%x).rstrip('0') MyPrint('\n Distances & angles for '+Oatom[1]+' at '+line.rstrip()) MyPrint(80*'*') line = '' for dist in Dist[:-1]: line += '%12s'%(AtomLabels[dist[0]].center(12)) MyPrint(' To cell +(sym. op.) dist. '+line.rstrip()) for i,dist in enumerate(Dist): line = '' for j,angle in enumerate(angles[i][0:i]): sig = angsig[i][j] if angle: if sig: line += '%12s'%(G2mth.ValEsd(angle,sig,True).center(12)) else: val = '%.3f'%(angle) line += '%12s'%(val.center(12)) else: line += 12*' ' if dist[4]: #sig exists! val = G2mth.ValEsd(dist[3],dist[4]) else: val = '%8.4f'%(dist[3]) tunit = '[%2d%2d%2d]'% dist[1] MyPrint((' %8s%10s+(%4d) %12s'%(AtomLabels[dist[0]].ljust(8),tunit.ljust(10),dist[2],val.center(12)))+line.rstrip()) def DisAglTor(DATData): 'Needs a doc string' SGData = DATData['SGData'] Cell = DATData['Cell'] Amat,Bmat = G2lat.cell2AB(Cell[:6]) covData = {} pfx = '' if 'covData' in DATData: covData = DATData['covData'] pfx = str(DATData['pId'])+'::' Datoms = [] Oatoms = [] for i,atom in enumerate(DATData['Datoms']): symop = atom[-1].split('+') if len(symop) == 1: symop.append('0,0,0') symop[0] = int(symop[0]) symop[1] = eval(symop[1]) atom.append(symop) Datoms.append(atom) oatom = DATData['Oatoms'][i] names = ['','',''] if pfx: names = [pfx+'dAx:'+str(oatom[0]),pfx+'dAy:'+str(oatom[0]),pfx+'dAz:'+str(oatom[0])] oatom += [names,] Oatoms.append(oatom) atmSeq = [atom[1]+'('+atom[-2]+')' for atom in Datoms] if DATData['Natoms'] == 4: #torsion Tors,sig = G2mth.GetDATSig(Oatoms,Datoms,Amat,SGData,covData) print ' Torsion angle for '+DATData['Name']+' atom sequence: ',atmSeq,'=',G2mth.ValEsd(Tors,sig) print ' NB: Atom sequence determined by selection order' return # done with torsion elif DATData['Natoms'] == 3: #angle Ang,sig = G2mth.GetDATSig(Oatoms,Datoms,Amat,SGData,covData) print ' Angle in '+DATData['Name']+' for atom sequence: ',atmSeq,'=',G2mth.ValEsd(Ang,sig) print ' NB: Atom sequence determined by selection order' else: #2 atoms - distance Dist,sig = G2mth.GetDATSig(Oatoms,Datoms,Amat,SGData,covData) print ' Distance in '+DATData['Name']+' for atom sequence: ',atmSeq,'=',G2mth.ValEsd(Dist,sig) def BestPlane(PlaneData): 'Needs a doc string' def ShowBanner(name): print 80*'*' print ' Best plane result for phase '+name print 80*'*','\n' ShowBanner(PlaneData['Name']) Cell = PlaneData['Cell'] Amat,Bmat = G2lat.cell2AB(Cell[:6]) Atoms = PlaneData['Atoms'] sumXYZ = np.zeros(3) XYZ = [] Natoms = len(Atoms) for atom in Atoms: xyz = np.array(atom[3:6]) XYZ.append(xyz) sumXYZ += xyz sumXYZ /= Natoms XYZ = np.array(XYZ)-sumXYZ XYZ = np.inner(Amat,XYZ).T Zmat = np.zeros((3,3)) for i,xyz in enumerate(XYZ): Zmat += np.outer(xyz.T,xyz) print ' Selected atoms centered at %10.5f %10.5f %10.5f'%(sumXYZ[0],sumXYZ[1],sumXYZ[2]) Evec,Emat = nl.eig(Zmat) Evec = np.sqrt(Evec)/(Natoms-3) Order = np.argsort(Evec) XYZ = np.inner(XYZ,Emat.T).T XYZ = np.array([XYZ[Order[2]],XYZ[Order[1]],XYZ[Order[0]]]).T print ' Atoms in Cartesian best plane coordinates:' print ' Name X Y Z' for i,xyz in enumerate(XYZ): print ' %6s%10.3f%10.3f%10.3f'%(Atoms[i][1].ljust(6),xyz[0],xyz[1],xyz[2]) print '\n Best plane RMS X =%8.3f, Y =%8.3f, Z =%8.3f'%(Evec[Order[2]],Evec[Order[1]],Evec[Order[0]]) def main(): 'Needs a doc string' arg = sys.argv if len(arg) > 1: GPXfile = arg[1] if not ospath.exists(GPXfile): print 'ERROR - ',GPXfile," doesn't exist!" exit() Refine(GPXfile,None) else: print 'ERROR - missing filename' exit() print "Done" if __name__ == '__main__': main()